Problem 31-2 Source:
Exercicie 17-3 - page 699 HAYT, William H. Jr. ,
KEMMERLY, Jack E. , DURBIN, Steven M. - Book: Análise de Circuitos em Engenharia -
Ed. McGraw Hill - 7ª Edição - 2008.
In the circuit shown in Figure 31-02.1, determine the parameters "Z".
Figure 31-02.1
Solution of the Problem 31-2
The Z parameters are given by the following equations:
V1 = Z11 I1 + Z12 I2
V2 = Z21 I1 + Z22 I2
We calculate Z11 when we do I2 = 0,
that is, an open circuit in port 2. Therefore, if there is no
current flowing at the exit of the quadripole, then Z11 will be the
serial-parallel association of the resistors that make up the circuit. Note that in
this case, resistor
of 20 ohms is in series with that of 5 ohms, having 25 ohms
as a result of the serial association. This association, in turn, is in parallel with
the resistor of 10 ohms. These three resistors result in an equivalent
resistance of:
The resistor of 40 ohms is in series with Req. Soon:
Z11 = 40 + Req = 40 + 7.143 = 47.143 Ω
To calculate Z22,
we should have I1 = 0. Then, looking at the output of the
quadripole, it is calculated
the resistance that the circuit presents when I1 = 0. Notice
that the reasoning is the same. In this case, the resistor of 20 ohms is in
series with that of 10 ohms and this set in parallel with that of
5 ohms . As a result, we obtain an equivalent resistance of:
Req = ( 30 x 5) / ( 30 + 5 ) = 150 /35 = 4.286 Ω
Likewise, the 40 ohms resistor is in series with Req, then:
Z22 = 40 + Req = 40 + 4.286 = 44.286 Ω
It's still missing to calculate Z12 and Z21.
To calculate
Z12 we should have I1 = 0 and we calculate the
relation V1 /I2.So, setting a value for
V2 and calculating V1 and I2,
as in the circuit shown ion the Figure 31-02.2, we get:
Figure 31-02.2
Note that we arbitrate a convenient value for V2 of 44.286 volts, because
we have already calculated the impedance Z22 = 44.286 Ω.
Thus, we easily calculate the value of I2, whose result is1 A. Knowing that
I1 = 0 and I2 = 1 A, we can find the value of V1,
because this will be the sum of the voltage drops in the resistors of 10
and 40 ohms, resulting the value of 41.43 volts .
To calculate V1, the current is calculated through the
20 ohms and 5 ohms resistors using a current divider. In the circuit
shown in the figure above, all the values are found. Now we can calculate
Z12, or:
Z12 = V1 /I2 = 41.43 /1 = 41.43 Ω
To calculate Z21 let's take the same procedure. For that, let's adopt
V1 = 47.143 volts. This value is convenient because we get I1 = 1 A.
Note that at 40 ohms resistor , it will also pass 1 A, causing a drop
of 40 volts on this resistor. Therefore, it is easy to calculate the other variables.
In the Figure 31-02.3, we see the values found.
Figure 31-02.3
Knowing that I1 = 1 A e V2 = 41.43 volts, then:
Z21 = V2 /I1 = 41.43 / 1 = 41.43 Ω
Note that Z12 = Z21 and with this, it is concluded that the circuit
is PASSIVE or RECIPROCAL.
Alternative Method
Another way to solve this problem is to use a Delta-Star transformation in
the set of resistors of 20 Ω , 10 Ω and 5 Ω that form a
Delta circuit.
So, starting from the circuit Delta shown in the Figure 31-02.4 and arriving at
the circuit Star shown in the Figure 31-02.5.
Figura 31-02.4Figura 31-02.5
Replacing this transformation in the original circuit, we have the circuit shown in the
Figure 31-02.6
Figure 31-02.6
Note that the value 41.43 is the result of the sum of 40 + 1.43 . Let's compare this circuit
with our model for reciprocal circuits that can be seen
in Theory. This way we can obtain
the following relations:
Z12 = 41.43 ohms
Z11 - Z12 = 5.715 ⇒ Z11 = Z12 + 5.715
When the calculation is made, we find the value of Z11, or:
Z11 = 41.43 + 5.715 = 47.145 ohms
On the other hand, it is known that:
Z22 - Z12 = 2.86 ⇒ Z22 = Z12 + 2.86
When the calculation is made, we find the value of Z22.
Z22 = 41.43 + 2.86 = 44.29 ohms
Note that these are the same values as previously found, unless numerical rounding.